American Mineralogist, Volume 66, pages 596-600, I98l Quartz with rhombohedralcleavagefrom Madagascar Orro W. FLORKE,HnrNz G. Mmrre, JtlncnN Wnrcnr,nt Institutfiir Mineralogie,Ruhr-UniversitritBochum,Postfach,D-4630Bochum,Germany AND HOLGER KULKE DEMINEX, DorotheenstraBe 1, D-4300Essen,Germany Abstrsct Anhedral quartz slabsfrom a vein depositin Madagascarshowingsmoothcleavageplanes parallel to positive rhombohedra r {l0ll) are described.Only two of the three equivalent pairs ofthe form {l0Tl} show cleavage,although ofdiflerent quality (smoothness).The best developedplaneslie parallel to Brazil-twin lamellae;the lesswell developedplanesdo not. We presumesmall tectonically induced thermal shocksto be the releasingmechanism for rhombohedral cleavagefractures. In combination with hydrolytic weakening and directed stress,large smoothcleavageplaneswere formed. Sincethe r-facesof quartz are F-faces,they have a minimum of free surfaceenergy.We assumethis to be the reasonfor cleavageparallel to positive rhombohedralfaces. Introduction Many authors describe qtrartz that, beyond its well-known conchoidalfracturing, under specialconditions shows cleavage of decreasing quality (smoothnessor perfection)on r {l0Tl}, z {0lTl}, and m {10T0}, respectively.In most caseshowever no distinction has been made betweenr and z. The cleavageparallel to ru usually is not well developed. Rose (1844) mentioned that cleavage of quartz may occur to an equal extent parallel to the positive and negativerhombohedra.The l9th century literature on quartz cleavage was reviewed by Hintze (1915), and the literature up to 1960 by Frondel (1962). All authors reported that pronounced platy cleavage or parting occasionally occurs in vein qtarlz, mostly in the inner parts of vein fillings. Rogers (1934) mentioned huge anhedral blocks of vein quartz from California pegmatites.Sinceparting wasnot observedparallel to all three equivalentpairs of rhombohedral faces, Rogers rejected the term cleavageand concludedthat parting might be due to polysyntheticDauphin6 1ryinning, mechanicallyproduced during the high-low transformation of the qvafiz. Murdoch and Webb (1938) describedquartz with nearly perfect platy parting in pegmatitic veins from another California localitv. The slabs showed flat 0003-004x/ 8| /0506-0s96$02.00 surfaceswith pearly luster over areasof l5 to 20 cm'z. Faint, unevenlyspaced,parallel striationsindicated a secondand a third direction of parting which were not as well developedas the first. Thin sectionscut normal to the principal parting plane showedparallel lamellae of varying width. The alternating arrangement of these lamellae resembled albite twinning. Therefore the authors concluded that this peculiar parting might be explained as a pseudomorph of single-crystalquartz after triclinic feldspar,though it was admitted that pseudomorphicreplacement by single crystalsinstead of fine-grainedpolycrystalline material is very unusual. Jahns (1953) stated that there existsno evidencethat large crystalsin pegmatites grow by replacementof other minerals. The production of cleavagein quartz through thermal shockby Kenngott (18M49) and under directed stressby Judd (1892) was mentioned by Hintze (1915).Borg and Maxwell (1956) subjectedqluartz sand to a directed stressof about 2 kbar at 300'C. under a confining pressureof about I kbar transmitted by alkaline hydrous solutions.They observed a remarkableincreaseof fracturing parallel to r and z, but none parallel to lrt. The percentageof grains with deformationlamellaedecreasedsimultaneously. The fractures occurred rarely in parallel setsand occasionallyconformedto more than one crystallographic plane. Bloss(1957)crushedquartz crystalsboth 596 FLORKE ET AL.: QUARTZ WITH RHOMBOHEDRAL CLEAVAGE at room temperature and between 650 and 700"C. tions perpendicularto the two recognizablecleavage He obtained a pronounced cleavageparallel to the planesweremeasuredto be 87!2". rhombohedra r and z and to a much lesser extent A systemofshort and lesslinsa1,healedfissuresM parallel to the prism m. also exists (Fig. 2). Angles of intersection between theseflssuresand R, or R,, are about 130to l40o in Geologicalsetting and mineralogy the same sectionsas above. The M-fissures.which One of us (HK) collected anhedral fragments of have healed after fracturing, representcharacteristic large single crystalswith almost perfect platy cleav- accumulations of aligned fluid inclusions. The Rage from qvartz veins in NE Madagascar.The hills, fracturesare unhealed. Universal-stagemeasurementsproved the R-fracbordering D'Antongil Baie (Fig. l) are part of an old tures to be the tracesof rhombohedralfacesand the cratonic block of Gondwana. Granites, migmatites M-fissures to be atgned almost parallel to prism and gneisseswere cut by a great number of quartz faces. veins and basalticdikes during the Late Cretaceous. At that time the separationof India from MadagasExperimentalresults car causedintenseshearingand mylonitization of the X-ray measurements,accordingto the orientation basementrocks (Hottin, 1969). Deep lateritic weatheringobscuresthe attitude and method of Keppler (1975),proved that the observed thicknessof the quartz veins. Furthermore, frequent cleavageplanesare rhombohedralfaces.It is difficult landslides have produced accumulations of quartz to distinguish between r- and z-rhombohedrausing blocks at the baseof the slopescontaining the origi- X-ray methods.Although the intensitiesof the reflections l0Tl and 0lTl are different (International Tanal outcrop. Our samplescome from quartz veins of about 2 m blesfor X-ray Crystalography,1969,Vol. I, p. 465) thickness, presumably crystallized from hydro- their exact determination is nearly impossible, bethermal solutions at the expenseof the quartz con- cause both reflections are strongly affected by extent ofthe shearedhost rocks.The quartz variesfrom tinction effects.Literature data (International Tables, milky or slightly smoky to absolutelytransparentin 1962,Yol. III, p. 79; Le Page et al., 1976)are convarious parts of the vein. Cleavageoccursespecially tradictory on the question of which reflection is the in the inner parts of the vein fi[ing. The remainder more intense. An unequivocal experimental indication of exhibits conchoidal fracturing only. The best developed cleavageswere observedin blocks of approxi- whether the rhombohedralcleavageplanesare posimately I m' volume composedof alnost clear quartz tive r- or negative z-planes (Bravais-setof crystalwith only minor trains of inclusions and cloudy lographic axes,seeDana Frondel, 1962)can be obtained by hydrothermal growth. Prisms measuring 5 schlieren(Fig. 2). x 5 x 15rrm were cut from platy fragmentswith two natural cleavageplanes forming two faces of these Sampledescription prisms. These served as seeds.Growth conditions Thin sectionsof various thicknessesproved the were: seedtemperature380oC,nutrient temperature samplesto be single crystals; however, the micro- 400"C, pressure1.5kbar, duration 14 days;nutrient: structure is characterizedby twin lamellae following broken quartz of the same sample, solvent: I m the Brazil law. Neighboring lamellae show differ- NarCO, in H, O. After the runs the seedcrystalswere encesin extinction position of 2o. The lamellaethem- terminatedonly by real facesm, r and z, with r promselves extinguish homogeneously.Specimens with inently developed parallel to the original cleavage macroscopicallyplanar cleavagesshow systemsof planesof the seed.The facesm and r were morpholong linear fractures parallel to the best developed logically dominant,whereasz-faceswere subordinate cleavageplanes.We refer to this fracture systemas due to their higher growth rate. The product crystals R,. The twin lamellae boundaries are frequently exhibited an unusual pseudoorthorhombic-prismatic identical with the R,-fractures.On the universalstage habit becauseof the prominent developmentof the a secondsystemof linear fractures,here termed R,r, rhombohedral faces. In agreement with literature running parallel to a secondpair of rhombohedral values,the measuredvelocitiesof growth VG were: faces r, could be measured.These fractures are sig- VG- < VG, << YG" (cf. Jost, 1955).Our growth exnificantly shorter than the R, type. The anglesof in- perimentsat different temperatures(pH ll, pressure tersectionbetweenfracture systemsR, and R,, in sec- 1.5to 3 kbar) show that in the temperaturerange up FLORKE ET AL.: QUARTZ WITH RHOMBOHEDRAL CLEAVAGE D E gronrtes t vetn w t t hc 1O81m , @ o o O t-t-t lO 2okm Fig. 1. Sketch of deposit, to 300oCthe free surfaceenergydifferencebetweenr and z is so large that z showsmuch higher growth rates than r. With increasingtemperature,however, the growth rates of r and z approacheach other and at 500"C thereis almostno differencebetweenthem. Twinning was analyzed by etching cuts perpendicularto the c-axis(45Vo}JF,20"C, 30 min), revealing polysyntheticBrazil twinrningparallel to only that rhombohedral face r which representsthe best developedcleavageplane. Untwinned, single crystal slabs(3-5 cm diameter) of transparent quartz fron diferent localities (Arkansas,Goiaz, Madagascar)were slowly heated(1"/ min) in air (l atm) to l00oC and subsequently quenchedin water to room temperature.After this procedure a few linear fractures parallel to the 'K' r{ \ '.1''-"# 1: 1, Rrt)*:.-o-', if *, .tI *, Fig. 2. Photomicrograph of linear rhombohedral cleavage fracture systems R1 and R1y and of healed fissures M; thin section cut perpendicular to the two macroscopic cleavage systems. FLORKE ET AL.: QUART:Z WITH RHOMBOHEDRAL CLEAVAGE rhombohedra were observed.When the maximum temperaturereached is increased,the fractures becamemore frequent but lesslinear. The reverseprocedure-shock heating and slow seeling to room temperature-resulted in the sameobservations. Completely different fractures were produced by shock heating to temperaturesabout the low-hightransformation of quartz. In this case the slabs cracked into a fabric of hexagonal, contiguous prisms, elongatedparallel to the c-axis. Even under hydrothermal conditions, as well as comparatively low ratesof heating and cooling the quartz shattered during the low-high-transformation. Discussionand conclusions The quartz cleavageparallel to the positive rhombohedron is in all casesobservedby us to be of different quality on the three equivalent pairs of the form {l0Tl}. One pair always showsthe best development of cleavageplanesand fractures(R). A second pair is of poorer cleavagequality (R,,). The third possiblesystemRr' was never observedin our samples. At standardtemperatureand pressure(25"C, I atm), and in the absenceof water, suitably oriented stressescaused samples with R-fractures to disintegrate into thin flakes parallel to these fracture planes,but they do not show any tendencyto form new ones. Under the as yet unknown natural conditions,the huge vein quartz crystalsunderwent an in situ cleaving processwithout the formation of deformation (Boehm) lamellae or deformation bands. The cleavagedescribedhere must be correlatedwith the structure of quartz.It requiresbreaking of the strong SiO-bonds in the tetrahedra-framework.Fairbairn (1939)calculatedthe number of Si-O-bonds per face unit and showedr and z to have a minimum, correspondingwith a minimum of coherenceof the corresponding lattice planes. Though he did not quantitatively discriminatebetweenr and z, he assumeda decreaseofcoherence in the sequence: o : {1120},c: {0001}, ffi, z, r. Fl6rke (1955,1959)describedthe positiverhombohedron as the only F-form, accordingto the PBC theory of Hartman and Perdoc (1955). In order to explain its morphologicalprominence,it must have the lowest free surfaceenergy,1.e.,a minillum of loose Si-O-bonds after cleavage.According to Hartman (1959), however, the z- and rz-faces should be Ffaces as well, but these do not show a comparable tendency to cleave. Hartman's method, though excellent,is a qualitative evaluationofsurface energies. Especiallyin complicatedstructureswith a complex bonding character,the results derived from it must be viewed with caution. The review of literature and our own experiments show that experimentally produced cleavage in qtartz, either by directed stressor by thermal shock without a hydrothermal confining pressure,is poor compared to the observednatural cleavage.Therefore we assume,without experimental evidence at present, that the coupled action of a directional stress,with the resolvedshear stressRSS exceeding the cleavagestresso" l0Tl, and a confining hydrothermal pressurehigh enough to initiate hydrolytic weakening (cf. Griggs, 1967) are necessaryto produce cleavagein quartz. We presume small tectonically induced thermal shocks(cf. Gay et al.,1978) under hydrothermal conditions in comparativelysmall volumes of the veinbearing rocks to be the releasing mechanism for cleavagein giant quartz crystals of suitable purity and suitable orientation relative to the stressdirections. From our experimental results we assumea rise of temperatureon the order of about l00oC to be necessary.We considerthe temperaturenot to have exceeded300"C. Due to the decreasingsurface energy differencesof r and z above300'C the tendency for cleavageshould not show significant differences. At higher temperatures,and especially above the low-high transformation temperature, we expect from our experimentalresultsthat evenunder hydrothermal conditions quafiz should shatterrather than cleave. The cleavagestrengtho" of the positive rhombohedral facesr at low temperatures(far below the lowhigh-transformation)is, from our undershlding of the quartz structure,lessthan it is for any other form and especially for the negative rhombohedron z. Thus the explosivetransformationof the storedstress energyinto surfaceenergyservesto form large, even smoothcleavageplanes.Additional hydrolytic weakening moreoverspecificallylowers the ideal and real cleavageenergyfor r by Si-O-bond breakingand activation of dislocationsin the structural framework. The proposedmechanismof cleavageaccountsfor both fracture and cleavagesystemsR' and Rrr, but it does not explain the di-fferencein cleavagequatty and the absenceof the symmetricallyequivalent system R,,,. We assumethis to be due to the polysynthetic Brazil twinning parallel to the best rhombohedralplane of cleavage.Brazil twinning along the 600 FLORKE ET AL.: QUARTZ WITH RHOMBOHEDRAL CLEAVAGE systemR,, doesnot occur. Twin boundariesare twodimensional areas of structural weakness.This causescleavageto be more easily achievedand explains the better cleavageof R, compared to R,,. Therefore we assumethe polysynthetic Brazil-twinning to have been formed before cleavage. Polysynthetic Brazil-twinning has been frequently observedin vein quartz (Frondel, 1962,p.87, Figs. 62, 63). The absenceof the third cleavagesystem R,,, is due to the orientation of the qvartz with regardto the directed stress.According to Schmid'slaw the shear stressr reachesa maximum at r-o* : o/2, if the angle betweenstresso and gliding plane happensto be 45o. The interfacial angle between two symmetrically equivalent rhombohedron faces r is 87". If the directed stresso. bisectsthe interfacial angle between two equivalent rhombohedron faces r, and r, the shear stressr nearly reachesa maximum for two planes at the sametime. The analogousorientation with regard to three equivalent rhombohedral faces rr, r, and rr, is, accordingto Schmid'slaw, difficult to realize.For only ong single orientation will the directedstressbe inclined at 45" to all three faces.The latter caseis lessprobable. Thus usually two rhombohedral cleavagesystemsare formed. Our understandingof rupture suggeststhat the distinction betweenfracture, parting and cleavagesuggestedby Fairbairn (1939) cannot be upheld. Even the conchoidalfracture of quartz is controlled by its structure (Hoffer, 196l). The term parting should be preserved for fractures controlled by segregation, zoning of impurities or exsolution (Buckley, 1934; White, 1979),whereascleavageshouldbe usedfor all planar fracturesof crystalswhich are intrinsically or primarily controlled by the structure. tobalit. Berichte der D€utschenKeramischenGesellschaft,32, 369-381. bei der paraFl6rke, O. W. (1959) Regelungserscheinungen morphen Umwandlung von SiO2-Kristallen. Zeitschrift fiir Kristallographie, ll2, 126-135. Frondel, C. (1945)Secondarydauphindtwinning in quartz. American Mineralogist,30, 47-460. Frondel, C. (1962)The systemof mineralogy.7. Ed. Vol. IIL Silica minerals,Wiley, New York, p. 104. Gay, N. C., Comins,N. R. and Simpson,C. (1978)The composition of spherules and shatter cone surfacesfrom the Vredefort structure,SouthAfrica. Earth and PlanetaryScienceLetters,41, 372-380. Griggs, D. (1967)Hydrolytic weakeningof quanz and other silicates.GeophysicalJournal of Royal Astronomical Society, 14, l9-3 l. Hartman, P. (1959)La morphologiestructuraledu quartz. Bulletin Soci€t€ Frangaisede Mineralogie et de Cristallographie, 82, 33s-340. Hartman, P. and Perdok, W. G. (1955)On the relations between structureand morphology of crystals,L Acta Crystallographica, 8.49-s2. Hintze, C. (1915) Handbuch der Mineralogie, 1. Band, 2. Abt., Veith & Co., Leipzig. Hoffer, A. (1961) Low quartz, on the geometry of its structure framework in terms of the directed bond. Zeitschrift ftir Kristallographie,I 16,83-100. Hottin, G. (1969)Les terrainscristallinedu Centreet du Nord-Est de Madagascar.Documentation du Bureau des G6ologiques, No. 178,Servaisg6ologiques,Tananarive. 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Maresch Ph.D., and we would like to express structureof low quartz. Acta Crystallographica,32,2456-59. our most sincere thanks to Mrs. Helene Nowara and Mr. Dieter Rogers,A. F. (1934) Unique occurrenceof vein quartz in MariDettmar for their valuable technical assistance. posa Country, California. Proceedingsof the Geological Society of America, 1934,327-328. References Rose,G. (18,t4)Uber das Kristallisationssystemdes Quarzes.AbBloss, F. D. (1957) Anisotropy of fracture in quartz. American handlungen der Akademischen Wissenschaften Berlin, PhysJournal of Science,255,214-225. 217-274, Tafel I-VI. ikalisch MathematischeKlasse,25.4.l 8214, Borg, I. Y. and Maxwell, J. C. (1956)Interpretation of fabrics of Strens,R. G. J. (1976)The physicsand chemistryof minerals and experimentally deformed sands. American Journal of Science, rocks. J. Wiley, London. 254, 7 r-81 . White, J. S. (1979)Boehmite exsolutionin corundum. American Buckley, H. E. (1934) On a cleavageinduced by impurity. Mineralogist,64, 1300-1302. Zeitschrift fUr Kristallographie(A), 88, 122-12'1. Fairbairn, H. W. (1939)Correlationof quartz deformationwith its crystal structure.American Mineralogist, 24, 351-368. Manuscript received, fune 16, 1980; Fl6rke, O. W. (1955) Strukturanomalienbei Tridymit und Crisaccepted for publication, January 5, I98I